<p>In this paper, we propose a new sixth-order weighted essentially non-oscillatory (WENO) scheme for solving compressible aerodynamics. As with the previous six-order central upwind WENO scheme, this present scheme is a convex combination of four linear reconstructions. The stencil type is the same as WENO-Z6 scheme (Hu FX <CitationRef CitationID="CR16">2018</CitationRef>), although the first three upwind stencils nominally use three cell values, the original secondary reconstruction has been modified to have fourth-order accuracy by adding a third-order correction term involving five cell values. In addition, corresponding smoothness indicators are provided, the new schemes are called WENO-MS-JS6 and WENO-MS-Z6. And by using the new reference smoothness indicator, the WENO-MS-Z6 scheme achieved the optimal convergence accuracy order in the smooth region including the first-order critical point (<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40314_2025_3144_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="159" /> </InlineMediaObject> <EquationSource Format="TEX">\(f^\prime _i=0,f^{\prime \prime }_i \ne 0, f^{\prime \prime \prime }_i \ne 0 \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>f</mi> <mi>i</mi> <mo>′</mo> </msubsup> <mo>=</mo> <mn>0</mn> <mo>,</mo> <msubsup> <mi>f</mi> <mi>i</mi> <mo>″</mo> </msubsup> <mo>≠</mo> <mn>0</mn> <mo>,</mo> <msubsup> <mi>f</mi> <mi>i</mi> <mrow> <mo>″</mo> <mo>′</mo> </mrow> </msubsup> <mo>≠</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>). Several numerical examples demonstrate that the new schemes have better resolution and the same robustness as the recently developed sixth order WENO schemes.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Improved sixth-order WENO scheme based on the numerical flux and smoothness indicators of modified stencils

  • Yahui Wang,
  • Guozeng Yang,
  • Cheng Guo,
  • Lijun Hu

摘要

In this paper, we propose a new sixth-order weighted essentially non-oscillatory (WENO) scheme for solving compressible aerodynamics. As with the previous six-order central upwind WENO scheme, this present scheme is a convex combination of four linear reconstructions. The stencil type is the same as WENO-Z6 scheme (Hu FX 2018), although the first three upwind stencils nominally use three cell values, the original secondary reconstruction has been modified to have fourth-order accuracy by adding a third-order correction term involving five cell values. In addition, corresponding smoothness indicators are provided, the new schemes are called WENO-MS-JS6 and WENO-MS-Z6. And by using the new reference smoothness indicator, the WENO-MS-Z6 scheme achieved the optimal convergence accuracy order in the smooth region including the first-order critical point ( \(f^\prime _i=0,f^{\prime \prime }_i \ne 0, f^{\prime \prime \prime }_i \ne 0 \) f i = 0 , f i 0 , f i 0 ). Several numerical examples demonstrate that the new schemes have better resolution and the same robustness as the recently developed sixth order WENO schemes.